<p>The <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11005_2025_1971_Article_IEq1.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="69" /> </InlineMediaObject> <EquationSource Format="TEX">\(GL_{\ell +1}(\mathbb {R})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>G</mi> <msub> <mi>L</mi> <mrow> <mi>ℓ</mi> <mo>+</mo> <mn>1</mn> </mrow> </msub> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="double-struck">R</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> Hecke-Baxter operator was introduced as an element of the <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11005_2025_1971_Article_IEq2.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="34" /> </InlineMediaObject> <EquationSource Format="TEX">\(O_{\ell +1}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>O</mi> <mrow> <mi>ℓ</mi> <mo>+</mo> <mn>1</mn> </mrow> </msub> </math></EquationSource> </InlineEquation>-spherical Hecke algebra associated with the Gelfand pair <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11005_2025_1971_Article_IEq3.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="126" /> </InlineMediaObject> <EquationSource Format="TEX">\(O_{\ell +1}\subset GL_{\ell +1}(\mathbb {R})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>O</mi> <mrow> <mi>ℓ</mi> <mo>+</mo> <mn>1</mn> </mrow> </msub> <mo>⊂</mo> <mi>G</mi> <msub> <mi>L</mi> <mrow> <mi>ℓ</mi> <mo>+</mo> <mn>1</mn> </mrow> </msub> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="double-struck">R</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>. It was specified by the property to act on an <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11005_2025_1971_Article_IEq2.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="34" /> </InlineMediaObject> <EquationSource Format="TEX">\(O_{\ell +1}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>O</mi> <mrow> <mi>ℓ</mi> <mo>+</mo> <mn>1</mn> </mrow> </msub> </math></EquationSource> </InlineEquation>-fixed vector in a <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11005_2025_1971_Article_IEq1.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="69" /> </InlineMediaObject> <EquationSource Format="TEX">\(GL_{\ell +1}(\mathbb {R})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>G</mi> <msub> <mi>L</mi> <mrow> <mi>ℓ</mi> <mo>+</mo> <mn>1</mn> </mrow> </msub> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="double-struck">R</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>-principal series representation via multiplication by the local Archimedean <i>L</i>-factor canonically attached to the representation. In this note we propose another way to define the Hecke-Baxter operator, identifying it with a generalized Whittaker function for an extension of the Lie group <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11005_2025_1971_Article_IEq6.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="158" /> </InlineMediaObject> <EquationSource Format="TEX">\(GL_{\ell +1}(\mathbb {R})\times GL_{\ell +1}(\mathbb {R})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>G</mi> <msub> <mi>L</mi> <mrow> <mi>ℓ</mi> <mo>+</mo> <mn>1</mn> </mrow> </msub> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="double-struck">R</mi> <mo stretchy="false">)</mo> </mrow> <mo>×</mo> <mi>G</mi> <msub> <mi>L</mi> <mrow> <mi>ℓ</mi> <mo>+</mo> <mn>1</mn> </mrow> </msub> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="double-struck">R</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> by a Heisenberg Lie group. We also show how this Whittaker function can be lifted to a matrix element of an extension of the Lie group <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11005_2025_1971_Article_IEq7.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="160" /> </InlineMediaObject> <EquationSource Format="TEX">\(Sp_{2\ell +2}(\mathbb {R})\times Sp_{2\ell +2}(\mathbb {R})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>S</mi> <msub> <mi>p</mi> <mrow> <mn>2</mn> <mi>ℓ</mi> <mo>+</mo> <mn>2</mn> </mrow> </msub> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="double-struck">R</mi> <mo stretchy="false">)</mo> </mrow> <mo>×</mo> <mi>S</mi> <msub> <mi>p</mi> <mrow> <mn>2</mn> <mi>ℓ</mi> <mo>+</mo> <mn>2</mn> </mrow> </msub> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="double-struck">R</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> by a Heisenberg Lie group.</p>

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The Hecke-Baxter operators via Heisenberg group extensions

  • A. A. Gerasimov,
  • D. R. Lebedev,
  • S. V. Oblezin

摘要

The \(GL_{\ell +1}(\mathbb {R})\) G L + 1 ( R ) Hecke-Baxter operator was introduced as an element of the \(O_{\ell +1}\) O + 1 -spherical Hecke algebra associated with the Gelfand pair \(O_{\ell +1}\subset GL_{\ell +1}(\mathbb {R})\) O + 1 G L + 1 ( R ) . It was specified by the property to act on an \(O_{\ell +1}\) O + 1 -fixed vector in a \(GL_{\ell +1}(\mathbb {R})\) G L + 1 ( R ) -principal series representation via multiplication by the local Archimedean L-factor canonically attached to the representation. In this note we propose another way to define the Hecke-Baxter operator, identifying it with a generalized Whittaker function for an extension of the Lie group \(GL_{\ell +1}(\mathbb {R})\times GL_{\ell +1}(\mathbb {R})\) G L + 1 ( R ) × G L + 1 ( R ) by a Heisenberg Lie group. We also show how this Whittaker function can be lifted to a matrix element of an extension of the Lie group \(Sp_{2\ell +2}(\mathbb {R})\times Sp_{2\ell +2}(\mathbb {R})\) S p 2 + 2 ( R ) × S p 2 + 2 ( R ) by a Heisenberg Lie group.